Final Magnetic Moment0.020 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom-0.189 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density9.28 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.000 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinFd3m [227] |
HallF 4d 2 3 1d |
Point Groupm3m |
Crystal Systemcubic |
Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
DyScO3 (mp-31120) | <0 1 0> | <1 1 0> | 172.1 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 121.7 |
Mg (mp-153) | <1 1 0> | <1 1 0> | 172.1 |
Mg (mp-153) | <1 1 1> | <1 0 0> | 121.7 |
GaP (mp-2490) | <1 0 0> | <1 0 0> | 121.7 |
GaP (mp-2490) | <1 1 0> | <1 1 0> | 172.1 |
TbScO3 (mp-31119) | <0 1 0> | <1 1 0> | 172.1 |
TbScO3 (mp-31119) | <1 1 0> | <1 0 0> | 121.7 |
NdGaO3 (mp-3196) | <0 0 1> | <1 0 0> | 121.7 |
NdGaO3 (mp-3196) | <0 1 0> | <1 1 0> | 172.1 |
NdGaO3 (mp-3196) | <1 0 0> | <1 1 0> | 172.1 |
NdGaO3 (mp-3196) | <1 1 0> | <1 0 0> | 121.7 |
Si (mp-149) | <1 0 0> | <1 0 0> | 121.7 |
Si (mp-149) | <1 1 0> | <1 1 0> | 172.1 |
ZrO2 (mp-2858) | <0 0 1> | <1 0 0> | 243.4 |
ZrO2 (mp-2858) | <1 0 0> | <1 1 0> | 172.1 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 121.7 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 172.1 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 172.1 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 121.7 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 172.1 |
CsI (mp-614603) | <1 0 0> | <1 0 0> | 121.7 |
CsI (mp-614603) | <1 1 0> | <1 1 0> | 172.1 |
SrTiO3 (mp-4651) | <0 0 1> | <1 0 0> | 121.7 |
SrTiO3 (mp-4651) | <1 1 0> | <1 0 0> | 121.7 |
LiAlO2 (mp-3427) | <0 0 1> | <1 0 0> | 243.4 |
CaF2 (mp-2741) | <1 0 0> | <1 0 0> | 121.7 |
CaF2 (mp-2741) | <1 1 0> | <1 1 0> | 172.1 |
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Nb3Co3C (mp-505601) | 0.1181 | 0.035 | 3 |
Co3Mo3N (mp-22166) | 0.1617 | 0.021 | 3 |
Mn3W3C (mp-15813) | 0.1765 | 0.000 | 3 |
Fe3W3N (mp-28452) | 0.1374 | 0.022 | 3 |
Fe3W3C (mp-20696) | 0.0183 | 0.035 | 3 |
Ti3Al2NiN (mp-542028) | 0.5741 | 0.000 | 4 |
Ti3Al2NiO (mp-628842) | 0.5955 | 0.295 | 4 |
Ta3Al2CoC (mp-510486) | 0.4961 | 0.000 | 4 |
Ti3Al2NiC (mp-505538) | 0.4912 | 0.000 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Fe_pv Mo_pv N |
Final Energy/Atom-9.6029 eV |
Corrected Energy-270.3257 eV
Uncorrected energy = -268.8817 eV
Composition-based energy adjustment (-0.361 eV/atom x 4.0 atoms) = -1.4440 eV
Corrected energy = -270.3257 eV
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Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)